Skip to content

Commit acb9af4

Browse files
author
Francisco Romero Hinrichsen
committed
README work
1 parent 77e7793 commit acb9af4

File tree

1 file changed

+27
-9
lines changed

1 file changed

+27
-9
lines changed

README.md

Lines changed: 27 additions & 9 deletions
Original file line numberDiff line numberDiff line change
@@ -49,21 +49,39 @@ Since measure spaces are in particular vector spaces, given a family of weights
4949
ω<sub>i</sub> >0, and a family of curves γ<sub>i</sub>, we can now consider μ,
5050
a weighted sum of these transported Dirac deltas
5151
<p align="center">
52-
<img src="https://github.com/panchoop/DGCG_algorithm/blob/assets/tex/eq_5.gif" width="150">
52+
<img src="https://github.com/panchoop/DGCG_algorithm/blob/assets/tex/eq_5.gif" width="140">
5353
</p>
5454
which is also a dynamic Radon measure.
5555

56+
The measures are "moving time continuously", but the measurements are gathered
57+
by sampling discretely in time. Fix those time samples as 0 = t<sub>0</sub> <
58+
t<sub>1</sub> < ... < t<sub>T</sub> = 1, then, at each time sample, the
59+
considered dynamic Radon measures are simply Radon measures. We therefore
60+
consider at each of these time samples t<sub>i</sub>, a forward operator
61+
mapping from the space of Radon measures, into some data space H<sub>i</sub>
5662

57-
![main_equation](https://github.com/panchoop/DGCG_algorithm/blob/assets/tex/eq_1.gif)
58-
59-
Given the considered penalizations, the obtained solution will be a
60-
*sparse* dynamic [Radon measure](https://en.wikipedia.org/wiki/Radon_measure), this is, a Radon measure with the
61-
following structure
63+
![eq_6](https://github.com/panchoop/DGCG_algorithm/blob/assets/tex/eq_6.gif)
64+
65+
Where at each time sample t<sub>i</sub>, the respective data spaces
66+
H<sub>i</sub> are allowed to be different. Theoretically, these data spaces
67+
are real [Hilbert spaces](https://en.wikipedia.org/wiki/Hilbert_space), numerically,
68+
these need to be finite dimensional.
69+
70+
Given data gathered at each time sample f<sub>0</sub> ∈ H<sub>0</sub>,
71+
f<sub>1</sub> ∈ H<sub>1</sub>, ... f<sub>T</sub> ∈ H<sub>T</sub>, and given
72+
any dynamical Radon measure ν, the data discrepancy term of our minimization
73+
problem is
6274

63-
![atoms](https://github.com/panchoop/DGCG_algorithm/blob/assets/tex/eq_2.gif)
75+
![eq_7](https://github.com/panchoop/DGCG_algorithm/blob/assets/tex/eq_7.gif)
6476

65-
that is a positively-weighted sum of Dirac deltas transported by curves the
66-
[Sobolev space](https://en.wikipedia.org/wiki/Sobolev_space#The_case_p_=_2) H<sup>1</sup>
77+
And putting together the data discrepancy term with the proposed
78+
energy J<sub>α, β</sub> to minimize, we build up the target
79+
functional that is minimized by our algorithm.
80+
81+
![main_equation](https://github.com/panchoop/DGCG_algorithm/blob/assets/tex/eq_1.gif)
82+
83+
The energy J<sub>α, β</sub> will promote sparse solutions μ, and the proposed
84+
algorithm will return one such measure.
6785

6886
To see an animated example of Dynamic sources, measured data, and obtained reconstructions,
6987
please see [this video](https://www.youtube.com/watch?v=daKkJZH3WD4).

0 commit comments

Comments
 (0)